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Water Drops and Cavitation Bubbles in Microgravity. 56th International Astronautical Congress 17th October 2005 , Fukuoka , Japan. D. Obreschkow, P. Kobel, N. Dorsaz, A. de Bosset, C. Nicollier, and M. Farhat. About cavitation. Cavitation bubbles. Damage. Concerned technologies. Implosion - PowerPoint PPT Presentation
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Water Drops and Cavitation Bubbles
in Microgravity
56th International Astronautical Congress17th October 2005, Fukuoka, Japan
D. Obreschkow, P. Kobel, N. Dorsaz, A. de Bosset,
C. Nicollier, and M. Farhat
About cavitation
Cavitationbubbles
Implosionphenomena
Concernedtechnologies
Damage
Goal
Confined shockwave
Observe all liquid jets
Interaction with spherical free surface
Water Drop
Cavitation Bubble
Here we go !
Part I
Water Drop
Drop Formation & Fixation
Drop Growth
10 mm
Drop Oscillations
1/e damp outtime = 0.7s
Drop-Electrodes Interaction
Negligible interaction
Repulsionby electrodes
Attractionby electrodes
Part II
Cavitation Bubble
It’s really fast !
Close-up
Stability of Drop and Free Surface
Counterjet Geometry
Planar free surface(ground experiment)
Spherical free surface(microgravity experiment)
bubble bubble
[Robinson et al. 01]
Free Surface
High pressure
Numerical Simulation
Shockwave-Nuclei Interaction
0.0ms 0.08ms 0.16ms
Shockwave Energy
Potential Energy
Evidence for “Hairjets”
= 0.95 (± 0.1)
Implosion Process
Modified Rayleigh-Plesset equation (empty bubble):
Rb(t)
Rd(t)
Conclusions
Direct Observation of Jet-Pair
Counterjet Geometry Change
Shockwave Confinement
Shockwave Energy Measurement
Stable Water Drop Formation
Damp Out Oscillations
FOLLOW-UP IDEAS: • Polarized Light (Schlieren) !• Higher time/space resolution• Smaller area of support
FLASH & SPLASH !
Appendix
Flight Maneuver
Global Evolution
Bubble inside extended volume on ground
Rayleigh-Plesset equation (empty bubble)